EP0573989B1 - Driving method for spatial light modulator - Google Patents
Driving method for spatial light modulator Download PDFInfo
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- EP0573989B1 EP0573989B1 EP93109300A EP93109300A EP0573989B1 EP 0573989 B1 EP0573989 B1 EP 0573989B1 EP 93109300 A EP93109300 A EP 93109300A EP 93109300 A EP93109300 A EP 93109300A EP 0573989 B1 EP0573989 B1 EP 0573989B1
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- Prior art keywords
- light modulator
- spatial light
- driving
- voltage
- time
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- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G3/00—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes
- G09G3/001—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes using specific devices not provided for in groups G09G3/02 - G09G3/36, e.g. using an intermediate record carrier such as a film slide; Projection systems; Display of non-alphanumerical information, solely or in combination with alphanumerical information, e.g. digital display on projected diapositive as background
- G09G3/003—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes using specific devices not provided for in groups G09G3/02 - G09G3/36, e.g. using an intermediate record carrier such as a film slide; Projection systems; Display of non-alphanumerical information, solely or in combination with alphanumerical information, e.g. digital display on projected diapositive as background to produce spatial visual effects
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/135—Liquid crystal cells structurally associated with a photoconducting or a ferro-electric layer, the properties of which can be optically or electrically varied
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- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G3/00—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes
- G09G3/001—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes using specific devices not provided for in groups G09G3/02 - G09G3/36, e.g. using an intermediate record carrier such as a film slide; Projection systems; Display of non-alphanumerical information, solely or in combination with alphanumerical information, e.g. digital display on projected diapositive as background
- G09G3/002—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes using specific devices not provided for in groups G09G3/02 - G09G3/36, e.g. using an intermediate record carrier such as a film slide; Projection systems; Display of non-alphanumerical information, solely or in combination with alphanumerical information, e.g. digital display on projected diapositive as background to project the image of a two-dimensional display, such as an array of light emitting or modulating elements or a CRT
Definitions
- the present invention relates to a driving method for a spatial light modulator which is to be used in a projection-type display, a holographic television set, an optical computer or the like.
- the driving pulses of the spatial light modulator are generally applied in synchronism with one frame cycle of the CRT.
- Such a driving method is reported, for example, in SID Digest (1991) Page 254--256. Timing charts for driving the CRT and spatial light modulator are shown in FIG.2.
- time-chart (a) shows the driving pulses of the CRT
- time-chart (b) shows the luminance intensity of a phosphor on the screen of the CRT
- time-chart (c) shows the driving signals of the spatial light modulator
- time-chart (d) shows the intensity of the output light from the spatial light modulator.
- the spatial light modulator is driven by the driving signals 204 which are applied in synchronism with the driving pulses 201 of the CRT.
- One driving signal 204 consists of an erasing pulse 202 and a reading period 203.
- a phosphor on the screen of the CRT When a phosphor on the screen of the CRT outputs a writing light 205 at a time in the reading time 203 of the driving signal 204, the light is received by a photo-conductive layer of a pixel of the spatial light modulator, the pixel of spatial light modulator turns on and starts up outputting an output light 206.
- the erasing pulse 202 is inputted to the spatial light modulator, the spatial light modulator turns off and the intensity of the output light 206 becomes zero.
- This method has the merit that the duty ratio of the output light (total on time of the output light in one frame cycle) can be made larger even when a material having a short life is used as a phosphor, and thereby a bright image can be obtained from the spatial light modulator.
- the spatial light modulator is turned on by an electric field generated by the negative voltage even when the writing light is not inputted thereto.
- the driving signals 204 have the wave forms shown in the time-chart (c) in FIG.2, so they do not apply any large negative voltage to the spatial light modulator. Therefore, the spatial light modulator may not turned on by the electric field and the image contrast ratio of the image is not reduced so much.
- half tone representation can be obtained by changing the luminance intensity of the phosphor on the CRT.
- a threshold voltage for switching the ferroelectric liquid crystal is varied by the amount of the accumulated ions.
- the threshold voltage is changed, deterioration appears in the switching characteristics of the ferroelectric liquid crystal with repetition of the driving.
- the wave forms of the driving signal are generally made to be symmetrical with respect to the polarity of voltage.
- time-chart (a) shows the wave form of the driving signal of the spatial light modulator
- time-chart (b) shows the intensity of the output light from the spatial light modulator.
- the driving signals are formed to be repetitions of an erasing pulse 301 and a writing pulse 302, and these two pulses 301 and 302 have substantially the same width and absolute value as the voltage but their polarities are opposite to each other.
- the output light is turned off without regard to the existence of the inputted light during the period of erasing pulse 301, and the output light is issued only when the inputted light exists during the period of writing pulse 302. Accordingly, the intensity of the output light 303 responding to the inputted light is shown by the time-chart (b) in FIG.3.
- FIG.4 shows another example of the driving signals.
- time-chart (a) shows the wave form of the driving signals of a spatial light modulator
- time-chart (b) shows the intensity of the output light from the spatial light modulator.
- one driving signal consists of an erasing pulse 401, a first lower voltage period 402, a writing pulse 403 and a second lower voltage period 404.
- the erasing pulse 401 and writing pulse 403 have substantially the same width and absolute value as the voltage but their polarities are opposite to each other.
- two lower voltage periods 402 and 404 have substantially the same width but their polarities are opposite to each other.
- FIG.5 Still another example of the driving signals of the spatial light modulator is shown in FIG.5.
- time-chart (a) shows the wave form of the driving signals
- time-chart (b) shows the intensity of the output light from the spatial light modulator.
- one driving signal consists of an erasing pulse 501, a first lower voltage period 502, a writing pulse 503 and a second lower voltage period 504.
- the duty ratio of the output light is at most 50%.
- the duty ratio of the intensity of output light 505 can be made nearly equal 1.
- the mean value of the intensity of the output light becomes larger and the contrast thereof is also increased.
- the driving signal becomes unsymmetrical to the time base, but the deterioration of the switching characteristics can be prevented even though the DC component of the driving signal averages out to be zero.
- a conductive material is used as the alignment film, the deterioration of the switching characteristics can be further prevented.
- the brightness of the screen is necessary to be completely uniform. It is, however, difficult to make the brightness of each part of the spatial light modulator completely uniform when the driving cycle of the spatial light modulator is completely in synchronism with the frame cycle of the CRT which is used as a writing means. Such a phenomenon is described referring to FIG.6.
- plan view (a) shows the scanning lines 601, 603 on a screen 605; time-chart (b) shows the wave form of the driving signal of the CRT and the spatial light modulator; time-chart (c) shows luminance intensity of a phosphor 602 on the screen 605; time-chart (d) shows the intensity of the output light from a pixel of the spatial light modulator corresponding to the phosphor 602; time-chart (e) shows luminance intensity of a phosphor 604 on the screen 606; and time-chart (f) shows the intensity of the output light from a pixel of the spatial light modulator corresponding to the phosphor 604.
- the screen 605 of CRT is scanned by electron beams, the phosphor 602, 604 which are irradiated by the electron beam output pulses of light, and thereby, an image is formed on the screen 605.
- the phosphor 602 which is positioned on an upper scanning line 601 outputs the light in an earlier time in the frame cycle of the CRT.
- the phosphor 604 which is positioned on a lower scanning line 602 outputs the light later than the phosphor 602.
- the reading time period 607 is made substantially equal to one frame cycle time of the CRT
- the light pulses from the phosphors 602 and 604 are respectively shown by the wave forms designated by numerals 608 and 610 in the time-charts (c) and (e) in FIG.6.
- the intensities of the output lights from the pixels of the spatial light modulator responding to the light pulses 608 and 610 respectively become the wave forms designated by numerals 609 and 611 in the time-charts (d) and (f) in FIG.6.
- the intensities of the light pulses 608 and 610 are substantially the same, the mean value of the intensity of the output light 611 becomes smaller than that of the output light 609 in the same frame cycle.
- the output light 611 is felt darker than the output light 609 by human eyes, and it is felt that the upper left portion of the screen 605 is brighter and the lower right portion is darker.
- the brightness of the output image from the spatial light modulator in each part becomes inhomogeneous.
- the objective of the present invention is to solve the above-mentioned problems and to provide an improved method for driving a spatial light modulator.
- a driving method for a spatial light modulator in accordance with the present invention is constituted that:
- the unit of driving voltage cycle consists of an erasing voltage time period and a writing voltage time period without interruption. Or, the unit of driving voltage cycle consists of an erasing voltage time period, a first lower voltage time period, a writing voltage time period and a second lower voltage time period.
- FIG.1 is a wave form illustration by means of time-charts, wherein (a) shows intensity of electron beams in a CRT; (b) shows luminance intensity of a phosphor on the CRT screen; (c) shows driving signals of a first preferred embodiment for driving a spatial light modulator; (d) shows intensity of output light from the spatial light modulator; (e) shows driving signals of a second preferred embodiment for driving the spatial light modulator; and (f) shows intensity of output light from the spatial light modulator in a driving method for a spatial light modulator in accordance with the present invention.
- FIG.2 is a waveform illustration by means of time-charts, wherein (a) shows the driving pulses of the CRT; (b) shows the luminance intensity of the phosphor on the CRT screen; (c) shows the driving signals of the spatial light modulator; and (d) shows the intensity of the output light from the spatial light modulator in a conventional driving method for a spatial light modulator.
- FIG.3 is a waveform illustration by means of time-charts, wherein (a) shows the driving signals of the spatial light modulator and (b) shows the intensity of the output lights from the spatial light modulator in another conventional driving method for a spatial light modulator.
- FIG.4 is a waveform illustration by means of time-charts, wherein (a) shows the driving signals of the spatial light modulator and (b) shows the intensity of the output lights from the spatial light modulator in still another conventional driving method for a spatial light modulator.
- FIG.5 is a waveform illustration by means of time-charts, wherein (a) shows the driving signals of the spatial light modulator and (b) shows the intensity of the output light from the spatial light modulator in still a further conventional driving method for a spatial light modulator.
- FIG.6(a) is the drawing showing the electron beam scanning on the CRT screen and time-charts at that time, wherein (a) schematically shows the scanning lines on the CRT screen 605; (b) shows the driving pulses of the CRT; (c) shows the luminance intensity of the phosphor 602; (d) shows the intensity of the output light from the pixel of the spatial light modulator corresponding to the phosphor 602; (e) shows the luminance intensity of the phosphor 604; and (f) shows the intensity of the output light from the pixel of the spatial light modulator corresponding to the phosphor 604.
- FIG.7 is a cross-sectional view showing an embodiment of a spatial light modulator driven by the driving method in accordance with the present invention.
- FIG.8 is a cross-sectional view showing another embodiment of a spatial light modulator driven by the driving method in accordance with the present invention.
- FIG.9 is a schematic drawing showing an optical system for evaluating a spatial light modulator driven by the driving method in accordance with the present invention.
- FIG.10 is a waveform illustration showing the relation between an embodiment of driving signals of a spatial light modulator and the intensity of output light from the spatial light modulator responding to the driving signals.
- FIG.11 is a waveform illustration showing the relation between another embodiment of driving signals of a spatial light modulator and the intensity of output light from the spatial light modulator responding to the driving signals.
- FIG.12 is a drawing showing the dependency of the intensities of output light from a spatial light modulator on the intensities of inputted light to the spatial light modulator.
- FIG.13 is a schematic drawing showing a projection-type display apparatus containing a spatial light modulator driven by the driving method in accordance with the present invention.
- FIG.14 is a schematic drawing showing a holographic television set including a spatial light modulator driven by the driving method in accordance with the present invention.
- the spatial light modulator 713 comprises: a transparent electrode 702 (which is made of, for example, ITO, ZnO, SnO 2 , or the like) formed on a transparent substrate 701 (which is made of, for example, glass or the like); a photo-conductive layer 706 with rectification formed on the transparent electrode 702; plural metal reflection film pixels 707 which are respectively independent from each other ((and made of, for example, Al, Ti, Cr, Ag, or lamination of at least two kinds of metals) formed on the photo-conductive layer 706; an alignment film 708 (which is made of, for example, high polymer film of polyimide or the like) formed on the metal reflection film pixels 707 for making a liquid crystal orient; another transparent electrode 711 (which is made of, for example, ITO, ZnO, SnO 2 or the like) formed on another substrate 712 (which is
- a part of the substrate 712, transparent electrode 702, photo-conductive layer 706, metal reflection film 707 and film 708 and another part of the substrate 712, transparent electrode 711 and film 710 are formed independently from each other. These two parts are fixed with a predetermined gap, and finally the ferroelectric liquid crystal 709 is filled in the gap.
- amorphous Si, Ge, Si1-xCx, Si1-xGex, Ge1-xCx (hereinafter, abbreviated as a-Si, a-Ge, a-Si1-xCx, a-Si1-xGex, a-Ge1-xCx) for the photo-conductive layer 706, hydrogen or halogen can be included therein.
- oxygen or nitrogen can be included for decreasing dielectric constant or increasing electrical resistivity.
- p-type impurities of B, Al, Ga or the like, or n-type impurities of P, As, Sb or the like can be added.
- Such an amorphous material to which the impurity is added can be laminated to form a junction of p/n, p/i, i/n, p/i/n or the like, and thereby, a depletion layer is formed in the photo-conductive layer for controlling the dielectric constant and dark resistivity or polarity of operating voltage of the photo-conductive layer.
- a depletion layer is formed in the photo-conductive layer for controlling the dielectric constant and dark resistivity or polarity of operating voltage of the photo-conductive layer.
- the amorphous material but also at least two other materials recited above can be laminated for forming a heterojunction structure in a manner to form the depletion layer in the photo-conductive layer.
- the thickness_of of the photo-conductive layer 706 is preferred to be from 0.1 to 10 ⁇ m.
- ITO thin film for the transparent electrode 702 is piled on a glass substrate 701 (which has dimensions of 40 mm ⁇ 40 mm ⁇ 1 mm) by sputtering.
- the thickness of the ITO film is about 1,000 angstroms.
- pin structure amorphous silicon (a-Si: H) for the photo-conductive layer 706 is piled on the transparent electrode 702 by plasma CVD method. Thicknesses of p-layer 703, i-layer 704 and n-layer 705 are respectively 1,000 angstroms, 17,000 angstroms and 2,000 angstroms, and total thickness of them is selected to be 2 ⁇ m.
- a material of p-layer 703 B (boron) is added in the amount of 400 ppm. And in the material of n-layer, P (phosphorus) is added in the amount of 400 ppm. In a material of i-layer 704, nothing is added.
- Cr film is formed on the entire surface of photo-conductive material 706 for forming metal reflection film pixels 707 by vacuum evaporation. After that, the Cr film is divided into minute pixels by photo-lithography. At this time, the size of each metal reflection film pixel 707 is 23 ⁇ m ⁇ 23 ⁇ m, and the gap between each pixel is 2 ⁇ m. Numbers of pixels are 1 ⁇ 10 6 (1,000 ⁇ 1,000).
- Polyamic acid is spread on the metal reflection film pixels 707 by a spin coat method, and the spread polyamic acid is hardened by heating. As a result, the polyimide alignment film 708 is formed. Thickness of the polyimide film is 100 angstroms. Orientation of the polyimide film 708 is generated by rubbing in one way by a nylon cloth.
- Another ITO transparent electrode 711 is similarly formed on another (glass) substrate 712, and another polyimide alignment film 710 is formed thereon and oriented. Furthermore, beads having a diameter of 1 ⁇ m are inlaid on the substrate 712 and fixed to the other substrate 701. Thereby, a gap of 1 ⁇ m is formed between both substrates 701 and 712. Finally, a ferroelectric liquid crystal 709 is filled in the gap, and the liquid crystal is heat treated. As a result, the spatial light modulator 713 is completely made.
- the spatial light modulator 817 is made in the following manner: a transparent electrode 803 formed on a transparent substrate 801; a photo-conductive layer 807 with rectification is formed on the transparent electrode 803 and includes a p-layer 804, an i-layer 805 and an n-layer 806; plural metal reflection films 810 which are respectively independent from each other are formed on the photo-conductive layer 807; a film 812 with an oriented structure is formed on the metal reflection film 810 for making a liquid crystal orient; another transparent electrode 813 is formed on another substrate 814; another alignment film 812 is spread on the transparent electrode 813; and a ferroelectric liquid crystal 811 is filled between the alignment films 812.
- a part designated by numeral 816 corresponds to a pixel of the spatial light modulator and a part designated by numeral 815 is a separation between the pixels.
- the spatial light modulator configured as shown in FIG.8 has essentially the same configuration of that shown in FIG.7, but has the following differences.
- Still another spatial light modulator (not shown in the figure) having a configuration that a conductive reflection film is entirely formed instead of the metal reflection film pixels 707 in FIG.7 is usable.
- time-chart (a) shows the intensity of electron beams of the CRT
- time-chart (b) shows the luminance intensity of phosphors on the CRT screen
- time-chart (c) shows the wave form of a first preferred embodiment of driving signals for driving the spatial light modulator
- time-chart (d) shows the intensity of output light from the spatial light modulator driven by the driving signals in the first embodiment
- time-chart (e) shows the wave form of a second preferred embodiment of driving signals for driving the spatial light modulator
- time-chart (f) shows the intensity of output light from the spatial light modulator driven by the driving signals in the second embodiment.
- a unit of a driving signal 107 shown in the time-chart (c) in FIG.1 is used as a driving signal.
- Such driving signals as shown in time-chart (c) in FIG.1 have repetition of the erasing pulse 105 and reading period (or writing period) 106.
- the erasing pulse 105 is inputted into a spatial light modulator wherein the photo-conductive layer with rectification and the ferroelectric liquid crystal are connected in series, the photo-conductive layer is forward-biased to be lower resistivity state. Therefore, the ferroelectric liquid crystal is forcibly turned off.
- the reading period 106 having a lower (negative) voltage the photo-conductive layer is reverse-biased.
- an intermediate polarization of the ferroelectric liquid crystal can be realized stably. It is considered that such intermediate polarization is realized by distribution of +P 0 state and -P 0 state in the liquid crystal or that the intermediate polarization is a transient state of turning the polarization of the liquid crystal.
- the intensity of output light from the spatial light modulator can be controlled by the quantity of photocurrent or intensity of the inputted light to the spatial light modulator, the half tone representation of an image on an output face of the spatial light modulator can be realized.
- the spatial light modulator is turned on by an electric field generated by a large negative voltage applied to the spatial light modulator.
- the contrast of the image decreases.
- the unit of driving signal 107 does not include any large negative voltage, the contrast of the image formed on the output face of the spatial light modulator does not decrease.
- the width of the erasing pulse 105 in the unit of driving signal 107 is made sufficiently narrow, the ratio of on state time of the spatial light modulator in the unit of driving signal 107 becomes large (that is, the duty ratio becomes large), and the time-averaged value of the output light 109 shown in the time-chart (6) in FIG.1 also becomes larger.
- the second preferred embodiment of the unit of driving signals 114 shown in time-chart (e) in FIG.1 can be used as driving signals for driving the spatial light modulator.
- the unit of the driving signal 114 consists of an erasing pulse 110, a first lower voltage period 111, a writing pulse 112 and a second lower voltage period 113.
- the unit of the driving signals 114 is considered as being formed by a writing pulse which is added over the driving pulse unit 107 shown in time-chart (c) in FIG.1. Since the driving pulse unit 114 is symmetrical with respect to the voltages, the mean value of the displacement of the ions becomes zero, even when the ions are generated in the liquid crystal by the high electric field.
- the threshold voltage of the liquid crystal does not change and the contrast of the image formed on the output face of the spatial light modulator does not change as time passes.
- the spatial light modulator can be driven stably. Still more, when the width of the second lower voltage period 113 is made wider than that of the first lower voltage period 111, the duty ratio of the output light becomes larger and thereby the contrast of the image also becomes larger.
- Time-chart (a) in FIG.1 shows the intensity of electron beam 103
- time-chart (b) shows the luminance intensity of the phosphor 104 on the CRT screen
- time-charts (c) and (e) show the wave forms of the driving signals 108 and 115
- time-charts (d) and (f) show the intensities of the output lights 109 and 116 from the spatial light modulator. Since the electron beams are scanned on the CRT screen, the electron beams reach a pixel on the CRT screen at interval of one frame cycle 102 of the CRT.
- the intensities of the electron beams 103 are in proportion to the brightness of a pixel of an image to be displayed in the CRT screen on the frame. Accordingly, the electron beams 103 having different intensities 101a, 101b, 101c... continuously reach each pixel at predetermined intervals.
- the phosphor on the CRT screen emits light with a luminance in proportion to the intensity of the electron beam 103 reaching it, and the intensity of emitted light from the phosphor damps with a predetermined time constant. Therefore, characteristic curves of the luminance intensity of the phosphor 104 shown in time-chart (b) in FIG.1 can be obtained.
- the intensity of output light 109 in each unit of driving signal 107 is in proportion to the luminance intensity of phosphor 104 at that time.
- the brightness of the image felt by human eyes, that is the mean value of output light 109 in one frame cycle 102 attains a value substantially in proportion to the luminance intensity of phosphor 104. Therefore, an image of high-fidelity can be reproduced on the spatial light modulator.
- the envelope which lines the peaks of the intensity of output lights 109 in respective units of driving signal 107 shown in the time-chart (d) in FIG.1 becomes closer to the shape of the luminance intensity of phosphor 104 as shown in time-chart (b) in FIG.1.
- the intensity of the output light 109 does not depend on the time difference between the driving signals 108 and the intensity of electron beam 103.
- the mean value of the output light 109 in one frame cycle 102 does not change so much. This means that the brightness of the output image from the spatial light modulator becomes uniform, since the intensity of output light 109 can be obtained with the same sensitivity against the intensity of the electron beams 103 at any part on the spatial light modulator.
- the optical system comprises a CRT 901, a spatial light modulator 902, a driving source 903 for driving the spatial light modulator, a beam splitter 904, a polarizer 905 and an analyzer 906.
- An input light 907 corresponding to an image from the CRT 901 is written in the spatial light modulator 902 from the photo-conductive layer side.
- the image is read out by the reading light 908 which is inputted through the analyzer 905 and beam splitter 904.
- the transmitting axes of the polarizer 905 and the analyzer 906 are perpendicular to each other.
- the spatial light modulator 902 is oriented in a manner so that it takes an extinctive position when the ferroelectric liquid crystal is off state.
- the spatial light modulator 902 one having a configuration shown in FIG.8 is used. It does not necessary whether the pitch of the pixels of CRT 901 is identical to, or different from the pitch of the pixels of the spatial light modulator 902. In this experiment, a CRT having 525 scanning lines with 50 ⁇ pixel pitch is used.
- an image-forming optical system such as a single lens or SELFOC (trade mark of Nippon Sheet Glass Company, Limited) lens array can be inserted between them.
- SELFOC trade mark of Nippon Sheet Glass Company, Limited
- the driving cycle of the spatial light modulator 902 is made shorter than the frame (for example, 1 msec).
- the CRT 901 and spatial light modulator 902 can be driven independently without synchronization at all, or they can be driven with synchronization in a manner so that a trigger pulse is generated and issued to the CRT 901 for every several driving pulses (for example, 16 pulses) of the spatial light modulator 902. In this optical system, the former is adopted.
- the spatial light modulator 902 was driven by using the driving signals 108 including many units of driving signal 107 shown in time-chart (c) in FIG.1 for reproducing the moving images on the CRT 901, and the output light from the spatial light modulator 902 was observed.
- a width of the erasing pulse 105 was 0.1 msec and its voltage was +10 V; the width of reading period 106 was 1.1 msec and its voltage was -0.91 V.
- one frame cycle of the CRT was 1.2 msec.
- the output light from the spatial light modulator 902 was directly observed through the beam splitter 904 by an observer 910.
- the spatial light modulator shown in FIG.7 has also been used in the afore-mentioned optical system shown in FIG.9 and the optical system has been driven similarly.
- the shielding of the reading light 908 was not sufficient, the brightness of the image was restricted to 1 ⁇ 10 3 lx.
- the other results have been substantially the same as those of the above-mentioned case of using the spatial light modulator shown in FIG.8.
- the driving signal 115 including a lot of units of driving signals 114 shown in the time-chart (e) in FIG.1 has been used for driving the afore-mentioned optical system shown in FIG.9.
- the width of erasing pulse 110 was 0.1 msec and its voltage was +10 V
- the width of the first lower voltage period 111 was 0.1 msec and its voltage has been 0 V
- the width of writing pulse 112 was 0.1 msec and its voltage was - 10 V
- the width of the second lower voltage period 113 was 0.9 msec and its voltage was 0 V.
- a spatial light modulator one having a configuration shown in FIG.8 was used.
- the image on the CRT 901 was faithfully reproduced so as to have brightness entirely uniform on the output face of the spatial light modulator 901. Furthermore, half-tone representation of the image was also reproduced and the residual image of the moving image was been observed on the output face of the spatial light modulator 901. The intensity of the output light from the spatial light modulator could have been increased to 1 ⁇ 10 6 lx.
- the phenomenon of switching the ferroelectric liquid crystal by the electric field due to the writing pulses 112 contained in the driving signals 115 occurred in this case, so that the contrast of the image on the output face of the spatial light modulator was inferior to that of the above-mentioned first experiment, and the contrast ratio was 80:1.
- the reproduced image was fit for observation. Since the driving signals 115 were symmetrical with respect to the polarity of the voltages, the stability of the spatial light modulator was improved even when the spatial light modulator has been continuously driven for dozens or so hours.
- the spatial light modulator shown in FIG.7 has also been used in the afore-mentioned optical system shown in FIG.9 and driven similarly.
- the brightness of the image has been restricted to 1 ⁇ 10 3 lx similar to the case of the first experiment.
- the results obtained have been similar to the case where the spatial light modulator shown in FIG.8 has been used.
- the characteristic curve designated by numeral 1004a is a case of using a writing light having an intensity of 3000 ⁇ W/cm 2
- the characteristic curve designated by numeral 1004b is a case of using a writing light having an intensity of 500 ⁇ W/cm 2
- the characteristic curve designated by numeral 1004c is a case of using no writing light. From FIG.10, it is found that when the intensity of the writing light is increased, the start up of the output light 1004 in the reading period 1002 becomes steep and mean value of the intensity of output light also becomes larger.
- the driving signal 1003 includes a erasing pulse 1001 and a reading period 1002.
- the driving signals 115 have been used for another experiment of examining the half-tone representation of the spatial light modulator.
- the result of the experiment is shown in FIG.11.
- the characteristic curve designated by numeral 1106a is a case of using a writing light having an intensity of 3000 ⁇ W/cm 2
- the characteristic curve designated by numeral 1106b is a case of using a writing light having an intensity of 500 ⁇ W/cm 2
- the characteristic curve designated by numeral 1106c is the case of using no writing light.
- the driving signals 1105 include an erasing pulse 1101, a first lower voltage period 1102, a writing pulse 1103 and a second lower voltage period 1104.
- FIG.11 shows that the half-tone representation can be obtained by changing the intensity of the writing light. Even when the writing light has been zero, a small peak appeared on the characteristic curve shown by numeral 1106c. This is due to the switching of the ferroelectric liquid crystal caused by the writing pulse 1103 with high negative voltage.
- characteristic curve 1201 shows the case of driving the spatial light modulator by using the driving signals not including writing pulse in one unit of driving signal, for example, 107 shown in time-chart (c) in FIG.1
- the other characteristic curve 1202 shows the case of driving the spatial light modulator by using the driving signals including a writing pulse 112 in one unit of driving signal, for example, 114 shown in time-chart (e) in FIG.1.
- the half-tone representation could be controlled when the intensity of the writing light is in a range from 100 to 1000 ⁇ W/cm 2 .
- the contrast ratio of the mean value of the intensity of the output light from the spatial light modulator is calculated as 53:1 in the case of using the driving signals 108, and as 32:1 in case of using the driving signals 115. The contrast ratios in both cases are satisfactory.
- the frequencies of the above-mentioned two driving signals have been changed without changing the waveforms and voltages of them for measuring the uniformity of the brightness of the output light in the optical system shown in FIG.9.
- the image displayed on the CRT screen 901 and having a uniform brightness was written in the spatial light modulator configured as shown in FIG.8.
- ratios R of the intensities of the darkest parts in the output side of the spatial light modulator 902 to those of the brightest parts have been calculated. The calculated ratios are shown in the following table 1.
- T SLM designates the period of the unit of driving signal of the spatial light modulator
- T CRT designates one frame cycle of the CRT
- R 1 and R 2 respectively designate the above-mentioned ratios of R when the spatial light modulator is driven by the driving signals 108 and 115 shown in FIG.1.
- T CRT is fixed to be 16.7 msec.
- T SLM (msec) T CRT /T SLM R 1 R 2 0.00835 2000 -- -- -- 0.0167 1000 1.0 1.0 0.167 100 1.0 1.0 1.67 10 1.1 1.1 8.35 2 1.2 1.3 11.1 1.5 2.1 2.0 16.7 1 11.3 12.7 33.4 0.5 -- --
- T CRT /T SLM when the value of T CRT /T SLM is in a range from 1.5 to 1000, the intensity of the output light becomes substantially uniform.
- the value of T CRT /T SLM is larger than 1000, the switching speed of the ferroelectric liquid crystal does not follow the change of the voltage of driving signals, so that the contrast of the image decreases.
- the value of T CRT /T SLM is smaller than 1, flicker of the output light becomes an eyesore, and thereby the quality of the image decreases.
- the widths of the erasing pulse 105 and reading period 106 were respectively fixed to be 0.1 msec and 1.1 msec, and only the voltages of them were changed for driving the spatial light modulator 817 shown in FIG.8.
- the quality of reproduced image did not decrease.
- the photo-conductive layer 807 of the spatial light modulator 817 shown in FIG.8 did not generate photocurrent in the reading period 106, so that the brightness of the output light from the spatial light modulator was reduced. Furthermore, in the case of fixing the voltage in the reading period 106 at -0.91 V and changing the voltage of erasing pulse 105 in a range from +2 V to +30 V, the quality of the reproduced image did not decrease so much.
- the photo-conductive layer 807 of the spatial light modulator 817 was forward-biased positively, so that the recorded information on the spatial light modulator 817 was not erased properly, and thereby the contrast of the image decreased.
- the spatial light modulator 817 shown in FIG.8 were driven by the driving signals 115 shown in time-chart (e) in FIG.1 deformed from those used in the afore-mentioned second experiment by changing one of the voltages among the erasing pulse 110, writing pulse 112 and second lower voltage period 113.
- a high quality image was obtained in a range from +2 V to +30 V for the same reason as the afore-mentioned case of changing the voltage of driving signals 108.
- a high quality image was obtained in a range from -30 V to -2 V.
- the optical system shown in FIG.9 has been attached to a projection type display which displays an expanded image.
- the elements in FIG.13 which are designated by the same numerals in FIG.9 are substantially the same, so that explanations of them are omitted.
- the output light from the optical system is enlarged and projected on a screen 1311 by a lens 1310.
- the area of the spatial light modulator 902 is 2.5 cm ⁇ 2.5 cm, but is enlarged to 100 cm ⁇ 100 cm on the screen 1311.
- the spatial light modulator 902 having substantially the same configuration as the spatial light modulator 816 shown in FIG.8 was driven by the driving signals 108 or 115 shown in the time-chart (c) or (e) in FIG.1, an image with high quality was obtained on the screen 1311.
- the illuminance on the screen 131 was 1,000 lx.
- the contrast ratio of the image on the screen 1311 was 100:1. Even though one pixel of the spatial light modulator 902 was expanded to 1 mm ⁇ 1 mm on the screen 1311, the crosstalk between the adjoining pixels was not observed and a fine image was obtained.
- three sets of the optical systems comprising the CRT 901 and spatial light modulator 902 respectively corresponding to the colors of red, green and blue could have been composed for superimposing the images on the screen 1311, thereby obtaining a color image.
- a holographic television set used a spatial light modulator 1410 having substantially the same configuration as shown in FIG.8.
- He-Ne laser 1401 is used for irradiating an object 1406.
- numerals 1402 designate reflection mirrors
- numerals 1403 designate half mirrors
- numerals 1404 designate lenses
- numerals 1405 designate collimators.
- the light beam through the object 1406 formed an interference fringe pattern on an image pickup surface of a CCD 1407 with reference light beam through the collimator 1405.
- Such image data formed on the CCD were transmitted to the CRT 1409 through a video signal transmission cable 1408.
- An image displayed on a screen of the CRT 1409 was focused on an input surface of the spatial light modulator 1410 by the focusing lens 1404. Therefore, the interference fringe pattern was inputted to the spatial light modulator 1410. Furthermore, the spatial light modulator 1410 reproduced the interference fringe pattern on an output face thereof. Coherent light from another He-Ne laser 1401' was used for reading out a stereoscopic image from the spatial light modulator 1410 in a reflection mode. The interference fringe pattern reproduced on the spatial light modulator 1410 was read out by the coherent reference light through a beam splitter 1411. Therefore, the stereoscopic image could be reproduced and observed by an observer 1412 in real time.
- the driving method for the spatial light modulator in accordance with the present invention is suitable to be used in the projection type display reproducing an image having high luminance, high resolution, high contrast, and half-tone representation. Furthermore, the holographic television set using the spatial light modulator driven by the driving method in accordance with the present invention can reproduce the real time stereoscopic image.
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- Computer Hardware Design (AREA)
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- Liquid Crystal (AREA)
Description
Accordingly, the
TSLM (msec) | TCRT/TSLM | R1 | R2 |
0.00835 | 2000 | -- | -- |
0.0167 | 1000 | 1.0 | 1.0 |
0.167 | 100 | 1.0 | 1.0 |
1.67 | 10 | 1.1 | 1.1 |
8.35 | 2 | 1.2 | 1.3 |
11.1 | 1.5 | 2.1 | 2.0 |
16.7 | 1 | 11.3 | 12.7 |
33.4 | 0.5 | -- | -- |
Claims (7)
- A method for driving a spatial light modulator,
comprising:providing a spatial light modulator having an output comprising a photo-conductive layer with rectification and a ferroelectric liquid crystal layer provided between a pair of transparent electrodes, with a side of the photo-conductive layer facing toward a light information inputting device having a predetermined frame cycle; andapplying plural units of a driving signal between said pair of transparent electrode during each frame cycle of the light information inputting device,so that output light intensity on the entire output face is substantially uniform. - The driving method for a spatial light modulator in accordance with claim 1, wherein
a ratio of a length of said unit of driving signal to a length of each said frame cycle is in a range from 1.5 to 1000. - The driving method for a spatial light modulator in accordance with claim 2, wherein
said unit of driving signal consists of an erasing voltage period and a writing voltage period. - The driving method for a spatial light modulator in accordance with claim 3, wherein
said erasing voltage is in a range from +2 V to +30 V and said writing voltage is in a range of -30 V to +2 V, wherein a direction of the voltage which biases said photo-conductive layer forward is defined to be positive. - The driving method for a spatial light modulator in accordance with claim 2, wherein
said unit of driving signal consists of a series of an erasing voltage period, a first lower voltage period, a writing voltage period and a second lower voltage period. - The driving method for a spatial light modulator in accordance with claim 5, wherein
a length of said second lower voltage period is longer than a length of said second lower voltage period. - The driving method for a spatial light modulator in accordance with claim 6, wherein
said erasing voltage is in a range from +2 V to +30 V, said writing voltage is in a range of -30 V to -2 V and voltage of said second lower voltage period is in a range from -2 V to +2 V, wherein a direction of the voltage which biases said photo-conductive layer forward is defined to be positive.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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JP151763/92 | 1992-06-11 | ||
JP15176392 | 1992-06-11 |
Publications (3)
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EP0573989A2 EP0573989A2 (en) | 1993-12-15 |
EP0573989A3 EP0573989A3 (en) | 1995-11-02 |
EP0573989B1 true EP0573989B1 (en) | 1998-09-16 |
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ID=15525766
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Application Number | Title | Priority Date | Filing Date |
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EP93109300A Expired - Lifetime EP0573989B1 (en) | 1992-06-11 | 1993-06-09 | Driving method for spatial light modulator |
Country Status (3)
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US (1) | US5416621A (en) |
EP (1) | EP0573989B1 (en) |
DE (1) | DE69321036T2 (en) |
Families Citing this family (11)
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JP3176661B2 (en) * | 1991-10-03 | 2001-06-18 | セイコーインスツルメンツ株式会社 | Optical writing spatial light modulator and sensitivity adjustment method thereof |
EP0642050B1 (en) * | 1993-09-02 | 2002-01-30 | Matsushita Electric Industrial Co., Ltd. | Spatial light modulator, method of production thereof and projection type display |
US5731797A (en) * | 1994-10-06 | 1998-03-24 | Matsushita Electric Industrial Co., Ltd. | Driving method for spatial light modulator and projection display system |
EP0752785A3 (en) * | 1995-07-03 | 1998-03-25 | Matsushita Electric Industrial Co., Ltd. | Video display device |
EP0762370A3 (en) * | 1995-08-02 | 1998-01-07 | Canon Kabushiki Kaisha | Driving method for display apparatus including an optical modulation device |
JPH09127544A (en) * | 1995-10-27 | 1997-05-16 | Matsushita Electric Ind Co Ltd | Projection type image display device |
EP0801321B1 (en) * | 1996-04-11 | 2002-08-21 | Matsushita Electric Industrial Co., Ltd. | Spatial light modulator and projector |
GB9622083D0 (en) * | 1996-10-23 | 1996-12-18 | Isis Innovation | 3-D image display |
GB2321754A (en) * | 1997-01-31 | 1998-08-05 | Sharp Kk | Diffractive spatial light modulator |
US6515310B2 (en) * | 2000-05-06 | 2003-02-04 | Semiconductor Energy Laboratory Co., Ltd. | Light-emitting device and electric apparatus |
DE102007018266A1 (en) * | 2007-04-10 | 2008-10-16 | Seereal Technologies S.A. | Holographic projection system with optical waveguide tracking and means for correcting the holographic reconstruction |
Family Cites Families (8)
Publication number | Priority date | Publication date | Assignee | Title |
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US4127322A (en) * | 1975-12-05 | 1978-11-28 | Hughes Aircraft Company | High brightness full color image light valve projection system |
US5130830A (en) * | 1989-02-27 | 1992-07-14 | Nippon Telegraph And Telephone Corporation | Spatial light modulator and spatial light modulating apparatus with alignment film having particular conductance |
US4941735A (en) * | 1989-03-02 | 1990-07-17 | University Of Colorado Foundation, Inc. | Optically addressable spatial light modulator |
JPH02260198A (en) * | 1989-03-31 | 1990-10-22 | Tokyo Noukou Univ | Liquid crystal electrooptical memory device |
JPH07104519B2 (en) * | 1990-01-12 | 1995-11-13 | セイコー電子工業株式会社 | Method for driving optical writing type liquid crystal light valve device |
EP0458270B1 (en) * | 1990-05-21 | 1996-11-27 | Victor Company Of Japan, Limited | Diplay unit |
JP2990297B2 (en) * | 1990-09-10 | 1999-12-13 | セイコーインスツルメンツ株式会社 | Liquid crystal light valve device and liquid crystal light valve driving method |
US5231282A (en) * | 1991-01-22 | 1993-07-27 | Mitsubishi Denki Kabushiki Kaisha | Optical writing type liquid crystal light valve and writing apparatus therefor |
-
1993
- 1993-06-08 US US08/073,060 patent/US5416621A/en not_active Expired - Fee Related
- 1993-06-09 DE DE69321036T patent/DE69321036T2/en not_active Expired - Fee Related
- 1993-06-09 EP EP93109300A patent/EP0573989B1/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
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EP0573989A3 (en) | 1995-11-02 |
DE69321036T2 (en) | 1999-02-18 |
EP0573989A2 (en) | 1993-12-15 |
DE69321036D1 (en) | 1998-10-22 |
US5416621A (en) | 1995-05-16 |
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